Coarse-graining support: #
Support.Sobolev.Foundations.CubeNeumannW22CZ.VectorFieldAndApex.BlockGlobalAndApex
Imported from the Apache-2.0 CoarseGraining development at commit
c7ddd76c08ade64fed1b8d2ca51be14dfee8deb4.
Compact-test weak equation on the full all-coordinate reflection block,
obtained by summing the single-cell weak equations over the finite 3^d
cell decomposition.
Compact-test weak equation on the full all-coordinate reflection block,
with the right-hand side given in the normalized cube L² measure used by the
endpoint interfaces.
Promote the reflected-block compact-test weak equation to a whole-space weak equation when the chosen test has zero contribution off the reflected block.
This is the interface used by the smooth Euclidean -Δu test: a mollified or
cutoff test supported inside the reflection block can be read as a global
compactly supported test on ℝ^d.
Whole-space reflected weak equation from pointwise zero of the test and its Euclidean gradient off the reflection block.
Whole-space reflected weak equation for compact smooth tests whose topological support is contained in the reflection block.
Whole-space reflected weak equation with the reflected forcing localized by
the reflection-block indicator. This is the global forcing form used by
Euclidean L² estimates.
The reflected Neumann gradient is L² on the full reflection block.
The block-indicator localization of the reflected Neumann gradient is a
global L² vector field.
Global reflected weak equation packaged with the global L² forcing
witness needed by Euclidean estimates.
Global reflected weak equation packaged with both global L² data: the
block-indicator reflected gradient and the block-indicator reflected forcing.
H10-test version of the reflected weak equation on the all-coordinate reflection block. This is the density bridge from the compact-test reflection identity to the Sobolev test space needed for the eventual reflected potential/limit argument.
Energy identity obtained by testing the reflected H10 weak equation against a supplied H10 potential for the reflected gradient. This isolates the next hard step: constructing such a potential for the reflected Neumann gradient.
Energy identity for the reflected block-folded H¹ potential. This avoids
any zero-trace claim: both sides are reduced by cell reflection to 3^d
copies of the original Neumann self-test identity on Q.
Smooth localized Euclidean CZ estimate obtained from the reflected weak equation, assuming the smooth potential has the reflected vector field as its gradient. This isolates the remaining density/mollification bridge.
Smooth localized Euclidean CZ estimate from the reflected weak equation, with the all-space reflected forcing norm converted back to the original cube forcing energy.
Smooth localized reflected Euclidean CZ estimate with the Laplacian factor cancelled on the Euclidean side.
Smooth localized reflected Euclidean CZ estimate with forcing energy converted back to the original cube.